Crystal Magnets for Refrigerator Set of 4, - Crystal Decor Magnetic Stones, Strong Office, Kitchen Fridge Magnet Set, Large Positive Energy Healing Crystals Gift Set (Multi - Unique Crystals)

£12.92
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Crystal Magnets for Refrigerator Set of 4, - Crystal Decor Magnetic Stones, Strong Office, Kitchen Fridge Magnet Set, Large Positive Energy Healing Crystals Gift Set (Multi - Unique Crystals)

Crystal Magnets for Refrigerator Set of 4, - Crystal Decor Magnetic Stones, Strong Office, Kitchen Fridge Magnet Set, Large Positive Energy Healing Crystals Gift Set (Multi - Unique Crystals)

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Duerrschnabel M, Yi M, Uestuener K, Liesegang M, Katter M, Kleebe HJ, Molina-Luna L. Atomic structure and domain wall pinning in samarium-cobalt-based permanent magnets. Nat Commun. 2017;8(1):54. Gutfleisch O, Müller KH, Khlopkov K, Wolf M, Yan A, Schäfer R, Schultz L. Evolution of magnetic domain structures and coercivity in high-performance SmCo 2:17-type permanent magnets. Acta Mater. 2006;54(4):997.

Liu JF, Ding Y, Zhang Y, Dimitar D, Zhang F, Hadjipanayis GC. New rare-earth permanent magnets with an intrinsic coercivity of 10 kOe at 500 °C. J Appl Phys. 1999;85(8):5660. Zhang TL, Liu HY, Liu JH, Jiang CB. 2:17-type SmCo quasi-single-crystal high temperature magnets. Appl Phys Lett. 2015;106(16):162403. Zhu MG, Sun W, Feng HB, Li Y, Fang YK, Zhou D, Li W. Effects of Sm content on thermal stability of Sm 2Co 17 sintered magnets. J Korean Phys Soc. 2013;63(3):784. Eldosouky A, Ikram A, Mehmood MF, Xu X, Šturm S, Rožman KŽ, Škulj I. Hydrogen decrepitation and spark plasma sintering to produce recycled SmCo 5 magnets with high coercivity. IEEE Magn Lett. 2018;9:1.Katter M, Weber J, Assmus W, Schrey P, Rodewald W. A new model for the coercivity mechanism of Sm 2(Co, Fe, Cu, Zr) 17 magnets. IEEE Trans Magn. 1996;32(5):4815.

Horiuchi Y, Hagiwara M, Okamoto K, Kobayashi T, Endo M, Kobayashi T, Sakurada S. Effect of pre-aging treatment on the microstructure and magnetic properties of Sm(Co, Fe, Cu, Zr) 7.8 sintered magnets. Mater Trans. 2014;55(3):482. Tang W, Zhang Y, Hadjipanayis GC. Effect of Zr on the microstructure and magnetic properties of Sm(Co balFe 0.1Cu 0.088Zr x) 8.5 magnets. J Appl Phys. 2000;87(1):399. Beketov VN, Moskalev VN, Taranov DV, Ogurtsov AV, Sharin MK, Popov AG, Terent’ev PB. Structure and properties of Sm–Co–Fe–Cu–Zr magnets for high-temperature applications. Met Sci Heat Treat. 2018;60(7–8):498. Huang G, Song XY, Liu D, Wang DX, Wang HB, Liu XM. Effects of Hf on phase structure and magnetic performance of nanocrystalline SmCo 7-type alloy. J Mater Sci. 2016;51(7):3390. Individual ions with fixed magnetic moments may cooperatively align their moments, resulting in the presence of magnetic properties of the crystal as a whole. Ferromagnet crystals have the magnetic moments from all their constituent ions aligned in the same direction; the magnetic moment of the crystal is the summation of the individual moments of the ions. There must be a magnetic force between the different ions that causes them to cooperatively align their moments. This force is also due to electron exchange. The d-orbitals from neighbouring ions overlap weakly into covalent bonds. The d-electrons on the separate ions are shared with the neighbour through covalent bonding. The electron exchange will tend to align the spins on the two neighbours. Aligning all pairs of neighbours aligns all ions. The exchange force between neighbours is much weaker than the force within the atomic shell of one ion. Although weak, the force is sufficient to cause ferromagnetism. Ferromagnetic materialsFerromagnetism is found in many insulators as well as metals. Chromium bromide (CrBr 3) is an insulator since chromium is trivalent and a bromine atom needs one electron to complete its outer shell. The trivalent chromium atoms each have a moment, and these align ferromagnetically below the Curie temperature of 37 K. Gadolinium chloride (GdCl 3; T c = 2.2 K) and europium oxide (EuO; T c = 77 K) are two other examples among many. Antiferromagnetic materials Zhang TL, Zhang B, Wang H, Jiang CB, Zhang ZH, Wang XQ, Zhang W. Low remanence temperature coefficient Sm 1− xEr x(Co, Fe, Cu, Zr) z magnets operating up to 400 °C. Rare Met. 2019. https://doi.org/10.1007/s12598-019-01223-4. Peng L, Yang QH, Zhang HW, Xu GL, Zhang M, Wang JD. Rare earth permanent magnets Sm 2(Co, Fe, Cu, Zr) 17 for high temperature applications. J Rare Earth. 2008;26(3):378.

Liu L, Liu Z, Li M, Lee D, Chen RJ, Liu J, Li W, Yan AR. Positive temperature coefficient of coercivity in Sm 1− xDy x(Co 0.695Fe 0.2Cu 0.08Zr 0.025) 7.2 magnets with spin-reorientation-transition cell boundary phases. Appl Phys Lett. 2015;106(5):052408.Superconducting Crystal Growth Magnets are used in the semi-conductor industry to improve the quality of monocrystalline silicon (mono-Si). Mono-Si is the basic material used in the production of integrated circuits. The application of a strong magnetic field during the growth of the larger diameter cylindrical ingots or boules of mono-Si reduces the incorporation of contaminants, thereby improving the quality of the resulting silicon crystal. Tesla Engineering has developed and supplies a portfolio of next generation superconducting Crystal Grower Magnets for the growth of monocrystalline silicon using the Czochralski method (MCZ). Tang W, Zhang Y, Hadjipanayis GC, Kronmüller H. Influence of Zr and Cu content on the microstructure and coercivity in Sm(Co balFe 0.1Cu yZr x) 8.5 magnets. J Appl Phys. 2000;87(9):5308. Liu JF, Ding Y, Hadjipanayis GC. Effect of iron on the high temperature magnetic properties and microstructure of Sm(Co, Fe, Cu, Zr) z permanent magnets. J Appl Phys. 1999;85(3):1670. Walmer MS, Chen CH, Walmer MH. A new class of Sm-TM magnets for operating temperatures up to 550 °C. IEEE Trans Magn. 2000;36(5):3376.



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